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1.
电阻焊质量稳定性试验是评价焊接设备性能的关键环节。由于影响接头质量稳定性的因素很多,因此试验难度大,失败率较高。本文从塑性环面积、工艺参数、气缸结构和试验方法等方面对影响点焊接头质量稳定性及其评价的因素进行了分析,并提出了有效的解决方案。  相似文献   

2.
通过对TC4钛合金旋压成形工艺技术的试验研究,分析了影响旋压成形和旋压件精度的因素,同时分析了旋压件的组织性能.试验结果表明,采用合理的旋压工艺及工艺参数,可以旋制较高精度的TC4钛合金零件,且旋压件材料组织性能提高,非金属成分含量仍满足标准要求.  相似文献   

3.
通过试验详细论述了不同锻造工艺对1Crl6CoSNi2MolWVNbN钢的金相组织、室温拉伸冲击性能、450℃拉伸性能和持久性能的影响。从而得出结论锻造工艺对合金室温和450℃拉伸性能、持久寿命影响不大,变形量的增加有利于细化晶粒和一次碳化物NbC的尺寸减小,在1120℃—l160℃始锻温度、40%~60%变形量条件下锻造合金室温冲击韧性处于较高水平。该合金的最佳锻造工艺参数为:1140℃下锻造,变形量50%左右。  相似文献   

4.
作者对带有光亮晶粒缺陷的L4M纯铝板进行了化学成分、金相分析、机械性能、冲压拉伸工艺、焊接和表面阳极化工艺试验;探讨了光亮晶粒的成因和性质。试验表明,纯铝板中的光亮晶粒对铝板的抗腐蚀性能几乎无影响,对焊接性能和表面阳极化无影响,机械性能有所下降。对于外观质量要求较高且必须采用拉伸变形工艺的工件,不宜采用这种带有光亮晶粒缺陷的铝板来制作。  相似文献   

5.
通过试验详细论述了不同锻造工艺对1Cr16Co5Ni2Mo1WVNbN钢的金相组织、室温拉伸冲击性能、450℃拉伸性能和持久性能的影响.从而得出结论锻造工艺对合金室温和450℃拉伸性能、持久寿命影响不大,变形量的增加有利于细化晶粒和一次碳化物NbC的尺寸减小,在1120℃~1160℃始锻温度、40% -60%变形量条件下锻造合金室温冲击韧性处于较高水平.该合金的最佳锻造工艺参数为:1140℃下锻造,变形量50%左右.  相似文献   

6.
新型卫星平台对具有较低热导率和较高尺寸稳定性的聚酰亚胺泡沫提出应用需求,为保证聚酰亚胺泡沫夹层结构胶接质量可靠性及工艺可实施性,需要对胶黏剂进行选型与性能评价。本文对硅橡胶(RTV-X,GD414)进行试验和讨论,通过胶黏剂力学性能、耐温性能、流变性能、90°剥离性能对比,确认RTV-X胶黏剂适用于聚酰亚胺泡沫夹层结构胶接工艺。通过分析验证确定胶接加压方式和胶接压力,并对试样进行高低温力学性能、温度冲击后力学性能考核,总结出以RTV-X为胶黏剂采取正压力≥1 kPa制备出的聚酰亚胺泡沫夹层结构胶接工艺可靠,制品胶接质量良好。所得结果可为深空探测等更多型号任务需求提供工艺参考。  相似文献   

7.
等离子喷涂参数对热障涂层热冲击性能的影响   总被引:2,自引:0,他引:2  
介绍了ZrO2热障涂层的等离子喷涂工艺及热冲击性能试验,通过不同工艺参数下的等离子喷涂工艺试验、金相分析、热冲击试验及扫描电子显微镜形貌分析,论述了喷涂电流及等离子气体流量对涂层热冲击性能的影响和试验结果对等离子喷涂ZrO2热障涂层的参数优化的重要意义。  相似文献   

8.
采用低频振动液体磨料研磨去毛刺工艺进行了去除微小孔钻削毛刺的试验。试验结果表明,该工艺方法能有效去除毛刺,具有工艺成本低,操作简便等优点,有较高的工程实用价值。  相似文献   

9.
一、引言 目前,我国航空工业正积极开展标准化工作,为了研制质量较高、工艺性较好的标准件,常常需要做对比试验。对于承受交变载荷的零件、构件,疲劳性能是重要的指标之一。利用对比试验,可以比较两种材料,两种工艺方法或两种构造形式等在疲劳性能方面哪一种较好,从而作为方案选择的依据。进行对比试验时,将待做对比的两组试件,在同一加载条件下(同一应力水平下),测定试件的疲劳寿命(破坏循环数)。根据对疲劳寿命观测值的统计分析,可以知道它们的疲劳性能是否相同,或者其中的一种疲劳性能优于另一种。  相似文献   

10.
利用自制的XMH-160型焊机对Ti-17合金进行了线性摩擦焊工艺试验,并对焊后试件进行了拉伸性能试验和接头组织分析.结果表明,接头的强度较高(接近母材),但塑性指标偏低;焊缝区为细条状且呈相间分布的α β细晶组织.通过对试件的拉伸断口进行分析,讨论了接头塑性指标偏低的主要原因.  相似文献   

11.
在Gleeble~1500热模拟实验机上,采用高温等温压缩,应变速率为0.001~10/s,变形温度为360~520%,对通用型铝锂合金在高温压缩变形中的流变应力行为进行了研究,分析了其高温变形的物理本质。结果表明:在等应变速率下,真应力随温度的升高而降低;在相同的变形温度下,随应变速率的增加,流变应力水平升高。在较低的变形速率及较高的变形温度条件下热变形时,通用型铝锂合金容易发生动态再结晶。而变形速率较高,变形温度较低时,通用型铝锂合金可能发生剪切变形,热变形过程中则主要发生动态回复。  相似文献   

12.
P2P模式的系统结构研究   总被引:15,自引:1,他引:15  
本文首先介绍了什么是P2P和它的基本运作模式。详细阐述P2P模式的主要形式及其相应的系统结构。  相似文献   

13.
Closed-form expressions are derived for the output noise response of an ?-?-? filter in steady-state operation with constant measurement noise statistics. To the author's knowledge such expressions have been unavailable until now. These formulas are useful for target tracking applications.  相似文献   

14.
针对我军用飞机大气数据计算机的测试问题,在全面分析了国产及俄制大气数据计算机测试需求的基础上,采用PCI总线技术,提出了一种满足系统测试需求的通用型硬件设计方案并自行研制开发了关键的硬件电路;在系统软件设计过程中采用面向对象设计思想,继承并封装了全部检测代码,根据测试需求分析的结果,修改、补充了新的属性和服务,增强了自动测试系统运行的稳定性和可靠性。  相似文献   

15.
干式切削是指高速切削金属时不使用冷却液的一种加工方法。本文介绍了高速干式加工工艺、技术特点及发展趋势。  相似文献   

16.
17.
We computed the evolution through case A mass transfer for 8 systems with mass of the primary equal to 3 and 5 M0, mass ratios 0.7 and 0.9, and different periods. To this we added similar results from Packet (1988) for Mi = 9 M0, qi = 0.6, Pi = 1.62 d.During the mass transfer two competing mechanisms in the gainer decide on the evolution of the system: the rejuvenation of this star as the increasing convective core mixes fresh hydrogen into the inner regions, and the acceleration of nuclear burning, responding to the increasing mass.In all the cases the net result is a faster decrease of the central hydrogen content compared to the mass losing star. The secondary fills its own critical Roche lobe and reversed mass transfer starts.From our results and those of Nakamura and Nakamura (1984), we find that reversed mass transfer occurs after core hydrogen burning of the secondary (case A1B2) approximately for periods larger than 1 d (M1i = 3 M0) to 2 d (M1i = 13.4 M0). For smaller periods this happens before the gainer ends its core hydrogen burning (case A1A2).  相似文献   

18.
MJS-8型30秒计时器,采用8051单片机,利用可编程通用,键盘和显示器接口器件8279来完成整个系统。本文主要介绍软件部分的设计。  相似文献   

19.
In part I (De Greve and Packet) we have investigated the occurrence of reversed phases of mass-transfer during Case A evolution in close binaries. If the initial period of a system is shorter than 1–2 days (Early Case A) the reversed phase starts before core hydrogen exhaustion of the gainer (part I). This type of evolution is characterized by at least two phases of slow mass-transfer.We have computed the evolution of four Early Case A systems with initial masses of the loser equal to 3 Mo and 5 Mo. These four systems start mass-exchange when Xc of the primary has decreased to 0.525 (75% of its initial value). They all experience two phases of slow mass-transfer.We find that both phases have about the same duration for all systems. The mass ratios are clearly distinct, being closer to unity during the first phase. In the Hertzsprung-Russell, mass-radius and mass-luminosity diagrams both components remain close to the main-sequence band during slow mass-transfer. Evolution as an Algol is ended when both components overflow their outer critical surface after a second reversal of the mass-transfer.Observed Algol systems evolving in Early Case A are scarce. A search thruogh the catalogue by Giuricin et al. gives us the following candidates: X Tri, SX Aur and V Pup. Based on their mass ratios, SX Aur can tentatively be assigned to the first phase of slow mass transfer and X Tri to the second phase. For V Pup (which is more massive) this choice can not be made with certainty.  相似文献   

20.
In part I (De Greve and Packet) we have investigated the occurrence of reversed phases of mass-transfer during Case A evolution in close binaries. If the initial period of a system is shorter than 1–2 days (Early Case A) the reversed phase starts before core hydrogen exhaustion of the gainer (part I). This type of evolution is characterized by at least two phases of slow mass-transfer. We have computed the evolution of four Early Case A systems with initial masses of the loser equal to 3 Mo and 5 Mo. These four systems start mass-exchange when Xc of the primary has decreased to 0.525 (75% of its initial value). They all experience two phases of slow mass-transfer. We find that both phases have about the same duration for all systems. The mass ratios are clearly distinct, being closer to unity during the first phase. In the Hertzsprung-Russell, mass-radius and mass-luminosity diagrams both components remain close to the main-sequence band during slow mass-transfer. Evolution as an Algol is ended when both components overflow their outer critical surface after a second reversal of the mass-transfer. Observed Algol systems evolving in Early Case A are scarce. A search thruogh the catalogue by Giuricin et al. gives us the following candidates: X Tri, SX Aur and V Pup. Based on their mass ratios, SX Aur can tentatively be assigned to the first phase of slow mass transfer and X Tri to the second phase. For V Pup (which is more massive) this choice can not be made with certainty.  相似文献   

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